A patent-citation network grows one patent at a time

PHYSICS · Subjective · Fermi University Physics · Thermal, Statistical & Complex Systems · Complex and collective systems · Complex and collective systems

Many Parts, One Behaviour, Ch Growing networks: preferential attachment and scale-free degree distributions

Problem

A patent-citation network grows one patent at a time, time tt counted in patents filed. Each new patent cites c=4c=4 earlier patents, chosen with probability proportional to qi+aq_i+a, where qiq_i is the number of citations patent ii has already received and a=8a=8 is a fixed offset that gives even an uncited patent (qi=0q_i=0) a nonzero chance of being cited. Let pqp_q be the stationary fraction of patents with exactly qq citations. (a) The total citation weight of all tt existing patents at time tt is ∑i(qi+a)=t(c+a)\sum_i(q_i+a)=t(c+a), since the total number of citations made is ctct. Using this, write the rate equation for Nq(t)N_q(t), substitute Nq=tpqN_q=tp_q, and show it reduces to pq=q−1+aq+a+1+a/c pq−1,q≥1.p_q=\frac{q-1+a}{q+a+1+a/c}\,p_{q-1},\qquad q\ge1. (b) The telescoping product of this recursion is a ratio of gamma functions recognisable as a beta function, pq∝B(q+a, 2+a/c)p_q\propto \mathrm{B}(q+a,\,2+a/c), whose large-qq behaviour B(x,y)∼Γ(y)x−y\mathrm{B}(x,y)\sim\Gamma(y)x^{-y} (quoted) gives a power-law tail pq∝q−γp_q\propto q^{-\gamma} with γ=2+a/c\gamma=2+a/c. Evaluate γ\gamma for this patent network. (c) Find the offset a′a' (at the same c=4c=4) that would instead reproduce the Barabási-Albert exponent γ=3\gamma=3, and comment on what the patent network's actual offset implies about its citation tail relative to a pure Barabási-Albert network.

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